Inward
Outward
Towards front
Towards back
1/m
V.R./m
m/V.R.
1/(m × V.R.)
ω
ωr
ω2r
ω/r
Newton
erg
kg-m
joule
Meet at one point, but their lines of action do not lie on the same plane
Do not meet at one point and their lines of action do not lie on the same plane
Meet at one point and their lines of action also lie on the same plane
Do not meet at one point, but their lines of action lie on the same plane
2.√(gh)
√(gh)
√(2gh)
2g.√h
Not a replace them by a single force
To replace them by a single force
To replace them by a single force through C.G.
To replace them by a couple
m₁. m₂. g/(m₁ + m₂)
2m₁. m₂. g/(m₁ + m₂)
(m₁ + m₂)/ m₁. m₂. g
(m₁ + m₂)/2m₁. m₂. g
2P sinθ/2
2P cosθ/2
2P tanθ/2
2P cotθ/2
Work is said to be done
Power is being transmitted
Body has kinetic energy of translation
None of these
π/16 (D² - d²)
π/16 (D³ - d³)
π/32 (D⁴ - d⁴)
π/64 (D⁴ - d⁴)
Angle between normal reaction and the resultant of normal reaction and the limiting friction
Ratio of limiting friction and normal reaction
The friction force acting when the body is just about to move
The friction force acting when the body is in motion
P = W tan (α - φ)
P = W tan (α + φ)
P = W tan (φ - α)
P = W cos (α + φ)
r/2
2r/3
r/A
3r/2
Meet in a point
Be all parallel
At least two of them must meet
All the above are correct
Maximum
Minimum
Zero
Infinity
P = mW - C
P = m/W + C
P = mW + C
P = C - mW
T.ω (in watts)
T.ω/60 (in watts)
T.ω/75 (in kilowatts)
T.ω/4500 (in kilowatts)
tan(α + φ)/tanα
tanα/tan (α + φ)
tan(α - φ)/tanα
None of these
Compression or tension
Buckling or shear
Shear or tension
All of the above
Three forces acting at a point will be in equilibrium
Three forces acting at a point can be represented by a triangle, each side being proportional to force
If three forces acting upon a particle are represented in magnitude and direction by the sides of a triangle, taken in order, they will be in equilibrium
If three forces acting at a point are in equilibrium, each force is proportional to the sine of the angle between the other two
Coefficient of friction
Angle of friction
Angle of repose
Sliding friction
Translatory
Rotary
Circular
Translatory as well as rotary
Distance moved by effort to the distance moved by load
Load lifted to the effort applied
Output to the input
All of the above
Same as
Twice
Thrice
Four times
The three forces must be equal
The three forces must be at 120° to each other
The three forces must be in equilibrium
If the three forces acting at a point are in equilibrium, then each force is proportional to the sine of the angle between the other two
20 N
40 N
120 N
None of these
Static friction
Dynamic friction
Limiting friction
Coefficient of friction
Output to the input
Work done by the machine to the work done on the machine
Mechanical advantage to the velocity ratio
All of the above
v = u + a.t
s = u.t + ½ a.t2
v2 = u2 + 2a.s
All of these